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青蛙骨骼肌中在高电压下动员的膜内电荷的特性和作用。

Properties and roles of an intramembranous charge mobilized at high voltages in frog skeletal muscle.

作者信息

Shirokova N, González A, Ma J, Shirokov R, Ríos E

机构信息

Department of Molecular Biophysics and Physiology, Rush University School of Medicine, Chicago, IL 60612, USA.

出版信息

J Physiol. 1995 Jul 15;486 ( Pt 2)(Pt 2):385-400. doi: 10.1113/jphysiol.1995.sp020820.

Abstract
  1. Membrane Ca2+ currents (ICa), intramembranous charge movement currents and changes in intracellular Ca2+ concentrations were recorded in voltage clamped cut skeletal muscle fibres of the frog. Intra- and extracellular solutions, designed to prevent ionic current, and use of the saponin-permeabilization procedure made possible the measurement of transfer of intramembranous charge up to high positive potentials. 2. Substantial charge moved at positive potentials. This charge was shown to be intramembranous in four tests of charge conservation, demonstrating that the total displacement of charge depended only on the initial and final voltages, and not on the history or pathway of intermediate voltages. 3. On average, in twenty-three cells, the charge moved at 50 mV was 31 +/- 1.9 nC microF-1 (mean +/- S.E.M.), and at 0 mV was 25 +/- 1.5 nC microF-1. Approximately one-fifth of the total charge moved above 0 mV. 4. The charge that moved at high voltage could be fitted, in most cases, with a Boltzmann distribution function. In twenty of twenty-three cells, the total charge distribution could be fitted as the sum of two Boltzmann terms; the high voltage term was centred at 11 +/- 3.9 mV, with a steepness factor of 12 +/- 1.6 mV and a magnitude of 8.6 +/- 1.1 nC microF-1. The low voltage term was centered at -43 +/- 2.1 mV, with a steepness factor of 7.7 +/- 0.6 mV and a magnitude of 22 +/- 1.8 nC microF-1. Thus, the high voltage component comprised about one-quarter of the mobile charge. In four cells it was possible to fit the sum of three Boltzmann terms to the distribution of mobile charge; the parameters of the high voltage term then were similar to those found by fitting the sum of two Boltzmann terms to the same data. 5. The voltage dependence of activation of ICa was determined in a buffered 2 mM Ca2+ external solution, from the tails of ionic current at -30 mV, after activating pulses to various voltages, the duration of which was sufficient to reach the peak of inward current. The voltage dependence was described by a Boltzmann function centred at 2.6 +/- 6.9 mV (n = 6), with a steepness factor of 20 +/- 1.4 mV. The voltages at which the high voltage charge moved were roughly the same as those at which ICa was activated. 6. Calcium release from the sarcoplasmic reticulum was determined from the Ca2+ transients. Calcium release continued to increase at potentials above 0 mV.(ABSTRACT TRUNCATED AT 400 WORDS)
摘要
  1. 在电压钳制的青蛙离体骨骼肌纤维中记录了膜钙电流(ICa)、膜内电荷移动电流和细胞内钙浓度的变化。设计用于防止离子电流的细胞内和细胞外溶液,以及使用皂素通透化程序使得在高达高正电位下测量膜内电荷转移成为可能。2. 在正电位下有大量电荷移动。在四项电荷守恒测试中表明该电荷位于膜内,这证明电荷的总位移仅取决于初始和最终电压,而不取决于中间电压的历程或路径。3. 平均而言,在23个细胞中,在50 mV时移动的电荷为31±1.9 nC μF⁻¹(平均值±标准误),在0 mV时为25±1.5 nC μF⁻¹。总电荷中约五分之一在0 mV以上移动。4. 在大多数情况下,在高电压下移动的电荷可以用玻尔兹曼分布函数拟合。在23个细胞中的20个中,总电荷分布可以拟合为两个玻尔兹曼项的总和;高电压项的中心位于11±3.9 mV,陡度因子为12±1.6 mV,幅度为8.6±1.1 nC μF⁻¹。低电压项的中心位于 -43±2.1 mV,陡度因子为7.7±0.6 mV,幅度为22±1.8 nC μF⁻¹。因此,高电压成分约占可移动电荷的四分之一。在四个细胞中,可以将三个玻尔兹曼项的总和拟合到可移动电荷的分布;然后高电压项的参数与通过将两个玻尔兹曼项的总和拟合到相同数据所发现的参数相似。5. 在缓冲的2 mM细胞外钙溶液中,通过在激活脉冲至各种电压后,从 -30 mV的离子电流尾电流中确定ICa激活的电压依赖性,激活脉冲的持续时间足以达到内向电流的峰值。电压依赖性由中心位于2.6±6.9 mV(n = 6)的玻尔兹曼函数描述,陡度因子为20±1.4 mV。高电压电荷移动的电压与ICa被激活的电压大致相同。6. 从钙瞬变确定肌浆网的钙释放。在高于0 mV的电位下钙释放持续增加。(摘要截断于400字)

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